Torque converter and system using the same

ABSTRACT

A torque converter device comprises a flywheel rotatable about a first axis, the flywheel including a first body portion having a first radius from a circumferential surface and a first radius of curvature, a first plurality of magnets mounted in the first body portion, each having first ends disposed from the circumferential surface of the first body portion, and each of the first ends of first plurality of magnets having a second radius of curvature similar to the first radius of curvature of the first body portion, a second plurality of magnets mounted in the first body portion, each of the second plurality of magnets being disposed from the circumferential surface of the first body portion, and a generator disk rotatable about a second axis angularly offset with respect to the first axis, the generator disk including a second body portion, and a third plurality of magnets within the second body portion for magnetically coupling to the first and second pluralities of magnets.

The present application is a Continuation-In-Part of U.S. patentapplication Ser. No. 10/758,000 filed on Jan. 16, 2004, which claimspriority to U.S. Provisional Patent Application No. 60/440,622 filed onJan. 17, 2003, which is hereby incorporated by reference.

BACKGROUND OF THE INVENTION

1. Field of the Invention

The present invention relates to a torque converter and a system using atorque converter. More specifically, the present invention relates to atorque converter that is capable of multiplying a given torque inputbased upon compression and decompression of permanent magnetic fields.In addition, the present invention relates to a system that uses atorque converter.

2. Discussion of the Related Art

In general, torque converters make use of mechanical coupling between agenerator disk and a flywheel to transmit torque from the flywheel tothe generator disk. However, due to frictional forces between thegenerator disk and the flywheel, some energy provided to the generatordisk is converted into frictional energy, i.e., heat, thereby reducingthe efficiency of the torque converter. In addition, the frictionalforces cause significant mechanical wear on all moving parts of thetorque converter.

SUMMARY OF THE INVENTION

Accordingly, the present invention is directed to a torque converterthat substantially obviates one or more of the problems due tolimitations and disadvantages of the related art.

An object of the present invention is to provide a torque converterhaving an increased output.

Another object of the present invention is to provide a system using atorque converter that reduces frictional wear.

Another object of the present invention is to provide a system using atorque converter that does not generate heat.

Another object of the present invention is to provide a system using atorque converter than does not have physical contact between a flywheeland a generator disk.

Another object of the present invention is to provide a system using atorque converter that allows an object to be inserted or reside betweena flywheel and a generator disk.

Additional features and advantages of the invention will be set forth inthe description which follows and in part will be apparent from thedescription, or may be learned by practice of the invention. Theobjectives and other advantages of the invention will be realized andattained by the structure particularly pointed out in the writtendescription and claims hereof as well as the appended drawings.

To achieve these and other advantages and in accordance with the purposeof the present invention, as embodied and broadly described, a torqueconverter device includes a flywheel rotating about a first axis, theflywheel having a first body portion having a first radius from acircumferential surface and have a first radius of curvature, a firstplurality of magnets mounted in the first body portion, each havingfirst ends disposed from the circumferential surface of the first bodyportion, and each of the first ends of first plurality of magnets havinga second radius of curvature similar to the first radius of curvature, asecond plurality of magnets mounted in the first body portion, each ofthe second plurality of magnets being disposed from the circumferentialsurface of the first body portion, and a generator disk rotatable abouta second axis angularly offset with respect to the first axis, thegenerator disk having a second body portion, and a third plurality ofmagnets within the second body portion for magnetic coupling with thefirst and second pluralities of magnets.

In another aspect, a torque converter device transferring rotationalmotion from a first body rotatable about first axis to a second bodyrotatable about and second axis angularly offset with respect to thefirst axis, the first and second bodies separated by a gap, one of thefirst and second bodies includes a first plurality of radially mountedmagnets, a plurality of backing plates, each disposed adjacent toinnermost end portions of the first plurality of magnets, and a magneticring disposed apart from each of the backing plates, wherein the backingplates are disposed between an end of the first plurality of radiallymounted magnets and the magnetic ring.

In another aspect, a method of transferring rotational motion from afirst body rotatable about a first axis to a second body rotatable abouta second axis angularly offset with respect to the first axis includessequentially compressing magnetic fields of a first plurality of magnetsradially mounted in the first body using at least one of a secondplurality of magnets mounted in the second body, and decompressing thecompressed magnetic fields of the first plurality of magnets as thefirst body and second body rotate to transfer the rotational motion ofthe first body to the second body.

In another aspect, a system for generating electrical power includes amotor, a flywheel rotating about a first axis, the flywheel having afirst body portion having a first radius from a circumferential surfaceand having a first radius of curvature, a first plurality of magnetsmounted in the first body portion, each having first ends disposed fromthe circumferential surface of the first body portion, and each of thefirst ends of first plurality of magnets having a second radius ofcurvature similar to the first radius of curvature, a second pluralityof magnets mounted in the first body portion, each of the secondplurality of magnets being disposed from the circumferential surface ofthe first body portion, and a generator disk rotatable about a secondaxis angularly offset with respect to the first axis, the generator diskhaving a second body portion, and a third plurality of magnets withinthe second body portion for magnetic coupling to the first and secondpluralities of magnets, and at least one electrical generator coupled tothe at least one generator disk.

It is to be understood that both the foregoing general description andthe following detailed description are exemplary and explanatory and areintended to provide further explanation of the invention as claimed.

BRIEF DESCRIPTION OF THE DRAWINGS

The accompanying drawings, which are included to provide a furtherunderstanding of the invention and are incorporated in and constitute apart of this application, illustrate embodiments of the invention andtogether with the description serve to explain the principles of theinvention. In the drawings:

FIG. 1A is a layout diagram of an exemplary flywheel according to thepresent invention;

FIG. 1B is a side view of an exemplary flywheel according to the presentinvention;

FIG. 1C is a side view of an exemplary attachment structure of theflywheel according to the present invention;

FIG. 2 is a perspective view of an exemplary retaining ring according tothe present invention;

FIG. 3 is an enlarged view of region A of FIG. 1A showing an exemplaryplacement of driver magnets within a flywheel according to the presentinvention;

FIGS. 4A and 4B are views of an exemplary driver magnet according to thepresent invention;

FIGS. 5A and 5B are views of another exemplary driver magnet accordingto the present invention;

FIGS. 6A and 6B are views of another exemplary driver magnet accordingto the present invention;

FIGS. 7A and 7B are views of another exemplary driver magnet accordingto the present invention;

FIG. 8A is a layout diagram of an exemplary generator disk according tothe present invention;

FIG. 8B is a side view of an exemplary shaft attachment to a generatordisk according to the present invention;

FIG. 9 is a schematic diagram of exemplary magnetic fields of theflywheel of FIGS. 1A-C according to the present invention;

FIG. 10 is a schematic diagram of an exemplary initial magneticcompression process of the torque converter according to the presentinvention;

FIG. 11A is a schematic diagram of an exemplary magnetic compressionprocess of the torque converter according to the present invention;

FIG. 11B is a schematic diagram of another exemplary magneticcompression process of the torque converter according to the presentinvention;

FIG. 11C is a schematic diagram of another exemplary magneticcompression process of the torque converter according to the presentinvention;

FIG. 11D is an enlarged view of region A of FIG. 11A according to thepresent invention;

FIG. 11E is another enlarged view of region A of FIG. 11A according tothe present invention;

FIG. 11F is another enlarged view of a region A of FIG. 11A according tothe present invention;

FIG. 12 is a schematic diagram of an exemplary magnetic decompressionprocess of the torque converter according to the present invention;

FIG. 13 is a schematic diagram of an exemplary magnetic force pattern ofthe flywheel of FIG. 1 during a magnetic compression process of FIG. 11according to the present invention;

FIG. 14 is a layout diagram of another exemplary flywheel according tothe present invention;

FIG. 15 is a layout diagram of another exemplary flywheel according tothe present invention;

FIG. 16 is a layout diagram of another exemplary flywheel according tothe present invention;

FIG. 17 is a schematic diagram of an exemplary system using the torqueconverter according to the present invention; and

FIG. 18 is a schematic diagram of another exemplary system using thetorque converter according to the present invention.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

Reference will now be made in detail to the illustrated embodiments ofthe present invention, examples of which are illustrated in theaccompanying drawings.

FIG. 1A is a layout diagram of an exemplary flywheel according to thepresent invention. In FIG. 1A, a flywheel 109 may be formed from acylindrical core of composite material(s), such as nylon, and may bebanded along a circumferential edge of the flywheel by a non-magneticretaining ring 116, such as non-magnetic stainless steel or phenolicmaterials. The flywheel 109 may include a plurality of magnets 102disposed within a plurality of equally spaced first radial grooves 101of the flywheel 109, wherein each of the magnets 102 may generaterelatively strong magnetic fields. In addition, each of the magnets 102may have cylindrical shapes and may be backed by a backing plate 203,such as soft iron or steel, disposed within each of the plurality offirst radial grooves 101 in order to extend the polar fields of themagnets 102 closer to a center C of the flywheel 109.

In FIG. 1A, the flywheel 109 may also include a plurality of suppressormagnets 108 disposed within a plurality of second radial grooves 107along a circumferential face of the flywheel 109. Accordingly, as shownin FIG. 3, surfaces 110 of the magnets 102 may be spaced from acircumferencial surface S of the flywheel 109 by a distance X, andsurfaces of the suppressor magnets 108 may be recessed from thecircumferencial face S of the flywheel 109 by a distance Y.

In FIG. 1A, each of the plurality of second radial grooves 107 may bedisposed between each of the plurality of first grooves 101. Forexample, each one of eight suppressor magnets 108 may be disposed withineach of eight grooves 107 and each one of eight magnets 102 may bedisposed within each of eight grooves 101. Accordingly, an angularseparation β between each of the first radial grooves 101 may be twicean angular separation a between adjacent first and second radial grooves101 and 107. Of course, the total number of magnets 102 and 108 and thefirst and second grooves 101 and 107, respectively, may be changed. Thesuppressor magnets 108 in the eight grooves 107 and the magnets 102 inthe eight grooves 101 of the flywheel 109 have their north magneticfields facing toward the circumferential surface S (in FIG. 3) of theflywheel 109 and their south magnetic fields facing radial inward towarda center portion C of the flywheel 109. Alternatively, opposite polararrangement may be possible such that the suppressor magnets 108 and themagnets 102 may have their south magnetic fields facing toward thecircumferential surface S (in FIG. 3) of the flywheel 109 and theirnorth magnetic fields facing radial inward toward a center portion C ofthe flywheel 109.

In FIG. 1A, backing plates 203 may be disposed at end portions of themagnets disposed within the plurality of first grooves 101 at the southpoles of the magnets 102 in order to form a magnetic field strengthalong a radial direction toward the circumferential surface S (in FIG.3) of the flywheel 109. Although not specifically shown, each of thebacking plates may be attached to the flywheel 109 using a fasteningsystem, such as retaining pins and/or bolts, or may be retained withinthe flywheel 109 due to the specific geometry of the magnets 102 withinthe first grooves 101. Accordingly, interactions of the magnetic fieldsof the magnets 102 within the plurality of first grooves 101 and thesuppressor magnets 108 disposed within the plurality of second grooves107 create a magnetic field pattern (MFP), as shown in FIG. 9, ofrepeating arcuate shapes, i.e., sinusoidal curve, around thecircumferential surface S (in FIG. 3) of the flywheel 109.

In FIG. 1A, the flywheel 109 may be formed of plastic material(s), suchas PVC and Plexiglas. In addition, the flywheel may be formed of moldedplastic material(s), and may be formed as single structure. The materialor materials used to form the flywheel 109 may include homogeneousmaterials in order to ensure a uniformly balanced system. In addition tothe circular geometry shown in FIG. 1A, other geometries may be used forthe flywheel 109. For example, polygonal and triangular geometries maybe used for the flywheel 109. Accordingly, the number of magnets 102 andthe suppressor magnets 108 and placement of the magnets 102 and thesuppressor magnets 108 may be adjusted to provide magnetic coupling to acorresponding generator disk 111 (in FIG. 8).

FIG. 1B is a side view of an exemplary flywheel according to the presentinvention. In FIG. 1B, the flywheel 109 may include first and secondbody portions 109 a and 109 b. Accordingly, the first and second grooves101 and 107 may be formed as semicircular grooves 101 a and 107 a in thefirst and second body portions 109 a and 109 b. In addition, althoughthe first and second grooves 101 and 107 are shown to be circular, othergeometries may be provided in order to conform to the geometries of themagnets 102 and the suppressor magnets 108.

In FIG. 1A, the total number of the magnets 102 and the suppressormagnets 108 may be adjusted according to an overall diameter of theflywheel 109. For example, as the diameter of the flywheel 109increases, the total number of magnets 102 and the suppressor magnets108 may increase. Conversely, as the diameter of the flywheel 109decreases, the total number of magnets 102 and the suppressor magnets108 may decrease. Furthermore, as the diameter of the flywheel 109increases or decreases, the total number of magnets 102 and thesuppressor magnets 108 may increase or decrease, respectively.Alternatively, as the diameter of the flywheel 109 increases ordecreases, the total number of magnets 102 and the suppressor magnets108 may decrease or increase, respectively.

FIG. 1C is a side view of an exemplary attachment structure of theflywheel according to the present invention. In FIG. 1C, the flywheel109 includes a fastening system having plurality of spaced fasteningmembers 122 that may be used to attach a major face of the flywheel 109to a shaft backing plate 120. Accordingly, a shaft 124 may be fastenedto the shaft backing plate 120 using a plurality of support members 126.In FIG. 1C, the shaft backing plate 120 may be formed having a circularshape having a diameter less than or equal to a diameter of the flywheel109. In addition, the shaft 124 may extend through the flywheel 109 andmay be coupled to an expanding flywheel 130. The expanding flywheel 130may be spaced from the flywheel 109 by a distance X in order to preventany deteriorating magnetic interference with the magnets 102 andsuppressor magnets 108 within the flywheel 109. The expanding flywheel130 may include structures (not shown) that would increase an overalldiameter D of the expanding flywheel 130 in order to increase theangular inertia of the flywheel 109. Moreover, the shaft 124 may extendthrough the expanding flywheel 130 to be supported by a supportstructure (not shown).

FIG. 2 is a perspective view of an exemplary retaining ring according tothe present invention. In FIG. 1A, the retaining ring 116 of theflywheel 109 may include a single band of stainless steel material, ormay include first and second retaining ring portions 116 a and 116 b,and may include attachment tabs 118 a, 118 b, and 118 d that attach tothe flywheel 109 via fasteners 118 c. The first retaining ring portion116 a may have outermost attachment tabs 118 a and innermost tabs 118 b,and the second retaining ring portion 116 b may have outermostattachment tabs 118 d and innermost tabs 118 b. In addition, as shown inFIG. 2, each of the attachment tabs 118 a, 118 b, and 118 d may includeattachment holes 318 for use with a fastener 118 c. Each of theattachment tabs 118 a, 118 b, and 118 d may be positioned within aregion between the first and second grooves 101 and 107. Although notspecifically shown, each of the attachment tabs 118 a, 118 b, and 118 dof the first and second retaining ring portions 116 a and 116 b may beformed to include two of the attachment holes 318 for use with twofasteners 118 c.

As shown in FIG. 1A, the first and second retaining ring portions 116 aand 116 b may cover the entire circumferential surface S (in FIG. 3) ofthe flywheel 109. Accordingly, the outermost attachment tabs 118 a ofthe first retaining ring portion 116 a and the outermost attachment tabs118 d of the second retaining ring portion 116 b may be fastened to theflywheel 109 at adjacent locations to each other. In addition, althougheach of the first and second retaining ring portions 116 a and 116 b areshown having three innermost attachment tabs 118 b, differentpluralities of the innermost attachment tabs 118 b may be used accordingto the size of the flywheel 109, the number of magnets 102 and 108, andother physical features of the flywheel 109 components within theflywheel 109.

Although not shown in FIG. 1A, a reinforced tape may be provided alongan outer circumference of the retaining ring 116. Accordingly, thereinforced tape may provide protection from abrasion to the retainingring 116.

FIG. 3 is an enlarged view of region A of FIG. 1A showing an exemplaryplacement of driver magnets within a flywheel according to the presentinvention. In FIG. 3, the surface 110 of the magnet 102 may have aradius of curvature R1 similar to the radius R2 of the flywheel 109. Forexample, R1 may be equal to R2, or R1 may be approximately equal to R2.In addition, the surface 108 a of the suppressor magnet 108 may have aradius of curvature R3 similar to the radiuses R1 and R2. However, thesurface 108 a of the suppressor magnet 108 may simply have a flat shape.

FIGS. 4A and 4B are views of an exemplary driver magnet according to thepresent invention. In FIG. 4A, the magnet 102 may have a first surface110 having the radius of curvature R1 that may be similar to the radiusR2 of the flywheel 109 (in FIG. 3). In addition, as shown in FIG. 4B,the magnet 102 may include a cylindrical side surface 130 that isconstant from a bottom surface 120 of the magnet 102 to the firstsurface 110 of the magnet 102.

FIGS. 5A and 5B are views of another exemplary driver magnet accordingto the present invention. In FIG. 5A, the magnet 202 may have a firstsurface 210 having the radius of curvature R1 that may be similar to theradius R2 of the flywheel 109 (in FIG. 3). In addition, as shown inFIGS. 4A and 4B, the magnet 202 may include a cylindrical side surface230 that is tapered from a bottom surface 220 of the magnet 202 to thefirst surface 210 of the magnet 202. Accordingly, the first grooves 101of the flywheel 109 may have corresponding sidewalls that conform to thetapered cylindrical side surface 230 of the magnet 202. In addition, theback plates 203 may also have corresponding tapered cylindrical surfacesas those of the magnet 202. However, the backing plates may not havetapered cylindrical surfaces as those of the magnet 202.

FIGS. 6A and 6B are views of another exemplary driver magnet accordingto the present invention. In FIG. 6A, the magnet 302 may have a firstsurface 310 having the radius of curvature R1 that may be similar to theradius R2 of the flywheel 109 (in FIG. 3). In addition, the magnet 302may have a shoulder portion 350 that transitions from a neck portion 340having a first diameter D1 to a body portion 330 having a seconddiameter D2. Furthermore, as shown in FIGS. 6A and 6B, the body portion330 of the magnet 302 may having a constant diameter D2 from a bottomsurface 320 of the magnet 202 to the shoulder portion 350 of the magnet302. Accordingly, the first grooves 101 of the flywheel 109 may havecorresponding portions that conform to the neck, shoulder, and bodyportions 340, 350, and 330 of the magnet 302.

FIGS. 7A and 7B are views of another exemplary driver magnet accordingto the present invention. In FIG. 7A, the magnet 402 may have a firstsurface 410 having the radius of curvature R1 that may be similar to theradius R2 of the flywheel 109 (in FIG. 3). In addition, the magnet 402may have a shoulder portion 450 that transitions from a neck portion 440having a first diameter D1 to a body portion 430 having a seconddiameter D2. Furthermore, as shown in FIGS. 7A and 7B, the body portion430 of the magnet 402 may having a constant diameter D2 from a bottomsurface 420 of the magnet 402 to the shoulder portion 450 of the magnet402. Accordingly, the first grooves 101 of the flywheel 109 may havecorresponding portions that conform to the neck, shoulder, and bodyportions 440, 450, and 430 of the magnet 402.

FIG. 8A is a layout diagram of an exemplary generator disk according tothe present invention. In FIG. 8A, a generator disk 111, preferably madefrom a nylon or composite nylon disk, may include two rectangularmagnets 301 opposing each other along a first common center line CL1through a center portion C of the generator disk 111, wherein each ofthe rectangular magnets 301 may be disposed along a circumferentialportion of the generator disk 111. In addition, additional rectangularmagnets 302 may be provided between the two rectangular magnets 301, andmay be opposing each other along a second common center line CL2 througha center portion C of the generator disk 111 that is perpendicular tothe first common center line CL1. Alternatively, the additionalrectangular magnets 302 may be replaced with non-magnetic weightedmasses in order to prevent an unbalanced generator disk 111.

In FIG. 8A, each of the two rectangular magnets 301, as well as each ofthe additional rectangular magnets 302 or the non-magnetic weightedmasses, may have a first length L extending along a directionperpendicular to the first and second common center lines CL1 and CL2,wherein a thickness of the two rectangular magnets 301, as well as eachof the additional rectangular magnets 302 or the non-magnetic weightedmasses, may be less than the first length L. In addition, each of thetwo rectangular magnets 301, as well as each of the additionalrectangular magnets 302, may have a relatively large magnetic strength,wherein surfaces of the two rectangular magnets 301, as well as each ofthe additional rectangular magnets 302, parallel to a major surface ofthe generator disk 111 may be one of south and north poles. Moreover,either an even-number or odd-number of magnets 301 may be used, andinterval spacings between the magnets 301 may be adjusted to attain adesired magnetic configuration of the generator disk 111.

FIG. 8B is a side view of an exemplary shaft attachment to a generatordisk according to the present invention. In FIGS. 8A and 8B, thegenerator disk 111 includes a plurality of spaced fastening members 305that may be used to attach the generator disk 111 to a shaft backingplate 306. Accordingly, a shaft 307 may be fastened to the shaft backingplate 306 using a plurality of support members 308. In FIG. 8B, theshaft backing plate 306 may be formed having a circular shape having adiameter less than or equal to a diameter of the generator disk 111.

In FIGS. 8A and 8B, the generator disk 111 may be formed of the same, ordifferent materials from the materials used to form the flywheel 109 (inFIG. 1A). Moreover, the geometry of the generator disk 111 may becircular, as shown in FIG. 8A, or may be different, such polygonal andtriangular shapes. In addition, the total number of the magnets 301, aswell as each of the additional rectangular magnets 302 or thenon-magnetic weighted masses, may be adjusted according to an overalldiameter of the flywheel 109 and/or the generator disk 111. For example,as the diameter of the flywheel 109 and/or the generator disk 111increases, the total number and size of the magnets 301, as well as eachof the additional rectangular magnets 302 or the non-magnetic weightedmasses, may increase. Conversely, as the diameter of the flywheel 109and/or generator disk 111 decreases, the total number and size of themagnets 301, as well as each of the additional rectangular magnets 302or the non-magnetic weighted masses, may decrease. Furthermore, as thediameter of the flywheel 109 and/or the generator disk 111 increases ordecreases, the total number and size of the magnets 301, as well as eachof the additional rectangular magnets 302 or the non-magnetic weightedmasses, may increase or decrease, respectively. Alternatively, as thediameter of the flywheel 109 and/or the generator disk 111 increases ordecreases, the total number and size of the magnets 301, as well as eachof the additional rectangular magnets 302 or the non-magnetic weightedmasses, may decrease or increase, respectively.

FIG. 9 is a schematic diagram of exemplary magnetic fields of theflywheel of FIG. 1 according to the present invention. In FIG. 9,interactions of the magnetic fields of the magnets 102 and thesuppressor magnets 108 create a magnetic field pattern (MFP) ofrepeating arcuate shapes, i.e., sinusoidal curve, around thecircumferential surface S of the flywheel 109. Accordingly, the backingplates 203 and the suppressor magnets 108 provide for displacement ofthe south fields of the magnets 102 toward the center C of the flywheel109.

FIG. 10 is a schematic diagram of an exemplary initial magneticcompression process of the torque converter according to the presentinvention, FIG. 11 is a schematic diagram of an exemplary magneticcompression process of the torque converter according to the presentinvention, and FIG. 12 is a schematic diagram of an exemplary magneticdecompression process of the torque converter according to the presentinvention. In each of FIGS. 10, 11, and 12, the schematic view is seenfrom a rear of the generator disk, i.e., the surface opposite to thesurface of the generator disk 111 having the two rectangular magnets301, and the flywheel 109 is located behind the generator disk 111. Inaddition, the flywheel 109 is rotating in a downward clockwise directionand the generator disk 111 is rotating along a counterclockwisedirection, wherein the generator disk 111 may be spaced from theflywheel 109 by a small air gap, such as within a range of aboutthree-eighths of an inch to about 0.050 inches. Alternatively, the smallair gap may be determined by specific application. For example, systemsrequiring a larger configuration of the flywheel and generator disk mayrequire larger or smaller air gaps. Similarly, systems requiring morepowerful or less powerful magnets may require air gaps having a specificrange of air gaps. Moreover, for purposes of explanation the magnets 102will now simply be referred to as driver magnets 102.

In FIG. 10, one of the two rectangular magnets 301 disposed on thegenerator disk 111 begins to enter one of the spaces within a magneticfield pattern (MFP) of the flywheel 109 between two north polesgenerated by the driver magnets 102. The driver magnets 102 may bedisposed along a circumferential center line of the flywheel 109, or maybe disposed along the circumference of the flywheel 109 in an offsetconfiguration. The gap between the driver magnets 102 in the flywheel109 is a position in which the MFP where the south pole field is theclosest to the circumferential surface S (in FIG. 9) of the flywheel109.

In FIG. 10, as the flywheel 109 rotates along the downward direction,the north pole of one of the two rectangular magnets 301 on thegenerator disk 111 facing the circumferential surface S (in FIG. 9) ofthe flywheel 109 enters adjacent north magnetic field lines of thedriver magnets 102 along a shear plane of the two rectangular magnets301 and the driver magnets 102. Accordingly, the shear force required toposition one of the two rectangular magnets 301 between the adjacentdriver magnets 102 is less than the force required to directly compressthe north magnetic field lines of the two rectangular magnets 301between the adjacent driver magnets 102. Thus, the energy necessary toposition one of the two rectangular magnets 301 between adjacent ones ofthe driver magnets 102 is relatively low.

In addition, the specific geometrical interface between the driver andrectangular magnets 102 and 301 provides for a relatively stablerepulsive magnetic field. For example, the cylindrical surface 130 (inFIG. 4) of the adjacent driver magnets 102, as well as the cylindricalsurfaces of the other exemplary driver magnets 202, 302, and 402 inFIGS. 5, 6, and 7, generate specific magnetic fields from the curvedsurfaces 110 and the bottom surfaces 120 of the driver magnets 102. Inaddition, the planar surfaces P (in FIG. 8) of the rectangular magnet301 entering the adjacent magnetic fields of the adjacent driver magnets102 generate another specific magnetic field. Accordingly, theinteraction of the magnetic fields of the driver and rectangular magnets102 and 301, and more specifically, the manner in which the magneticfields of the driver and rectangular magnets 102 and 301 are broughtinto interaction, i.e., along a magnetic shear plane, create arelatively stable repulsive magnetic field.

In addition, although the suppressor magnet 108 also provides arepelling force to the driver magnet 102, the force of repulsion of thesuppressor magnet 108 is relatively less than the repulsive force of therectangular magnet 301. However, as will be explained with regard toFIG. 12, the suppressor magnet 108 provides an additional repulsionforce when the magnetic fields of the driver and rectangular magnets 102and 301 are decompressed.

In FIG. 11A, once the rectangular magnet 301 on the generator disk 111fully occupies the gap directly between the north poles of two adjacentdriver magnets 102 of the flywheel 109, the weaker north pole (ascompared to the north poles of the driver and rectangular magnets 102and 301) of the suppressor magnet 108 on the flywheel 109 is repelled bythe presence of the north pole of the rectangular magnet 301 on thegenerator disk 111. Thus, both the north and south magnetic fields ofthe MFP below the outer circumference of the flywheel 109 arecompressed, as shown at point A (in FIG. 13).

In FIG. 11A, a centerline CL3 of the flywheel 109 is aligned with acenterline CL4 of the magnet 301 of the generator disk 111 duringmagnetic field compression of the driver magnets 102, the suppressormagnet 108, and the magnet 301 of the generator disk 301. Accordingly,placement of the rotation axis of the flywheel 109 and the rotation axisof the generator disk 111 must be set such that the centerline CL3 ofthe flywheel 109 is aligned with the centerline CL4 of the magnet 301 ofthe generator disk 111.

However, as shown in FIGS. 11B and 11C, placement of the rotation axisof the flywheel 109 and the rotation axis of the generator disk 111 maybe set such that the centerline CL3 of the flywheel 109 may be offsetfrom the centerline CL4 of the magnet 301 of the generator disk 111 by adistance X. Accordingly, the magnetic field compression of the drivermagnets 102, the suppressor magnet 108, and the magnet 301 of thegenerator disk 301 may be altered in order to provide specific repulsionforces between the driver magnets 102, the suppressor magnet 108, andthe magnet 301 of the generator disk 301.

FIG. 11D is an enlarged view of region A of FIG. 11A according to thepresent invention. In FIG. 11D, a distance X between facing surfaces ofthe driver magnet 102 (and likewise the other driver magnet 102 adjacentto the opposing end of the magnet 301 of the generator disk 111) is setin order to provide specific magnetic field compression of the drivermagnets 102 and the magnet 301 of the generator disk 111. Preferably,the distance X may be set to zero, but may be set to a value to ensurethat no torque slip occurs between the flywheel 109 and the generatordisk 111. The torque slip is directly related to the magnetic fieldcompression strength of the driver magnets 102 and the magnet 301, aswell as the magnetic strength and geometries of the driver magnets 102and the magnet 301.

FIG. 11E is another enlarged view of region A of FIG. 11A according tothe present invention. In FIG. 11, the driver magnet 102 may have across-sectional geometry that includes a polygonal shape, wherein a sideof the polygonal shaped driver magnet 102 may be parallel to a side ofthe magnet 301 of the generator disk 11. However, the distance X betweenfacing surfaces of the driver magnet 102 (and likewise the other drivermagnet 102 adjacent to the opposing end of the magnet 301 of thegenerator disk 111) is set in order to provide specific magnetic fieldcompression of the driver magnets 102 and the magnet 301 of thegenerator disk 111. Preferably, the distance X may be set to zero, butmay be set to a value to ensure that no torque slip occurs between theflywheel 109 and the generator disk 111.

FIG. 11F is another enlarged view of a region A of FIG. 11A according tothe present invention. In FIG. 11F, pairs of driver magnets 102 a and102 b may be provided in the flywheel 109. The driver magnets 102 a and102 b may be provided along centerlines CL3A and CL3B, respectively, andmay be spaced apart from the centerline CL3 of the flywheel 109, as wellas the aligned centerline CL4 of the magnet 301 of the generator disk111. Accordingly, the magnetic field compression of the pair of drivermagnets 102 a and 102 b and the magnet 301 of the generator disk 301 maybe altered in order to provide specific repulsion forces between thepair of driver magnets 102 a and 102 b, the suppressor magnet 108, andthe magnet 301 of the generator disk 301. As with the polygonal shapedgeometry of the single driver magnets 102, in FIG. 11E, the pair ofdriver magnets 102 a and 102 b may have polygonal shaped geometries. Inaddition, similar to the distance X, as shown in FIGS. 11D and 11E,distances between facing surfaces of the pair of driver magnets 102 aand 102 b (and likewise the other pair of driver magnets 102 a and 102 badjacent to the opposing end of the magnet 301 of the generator disk111) is set in order to provide specific magnetic field compression ofthe pair of driver magnets 102 a and 102 b and the magnet 301 of thegenerator disk 111. Preferably, the distance X may be set to zero, butmay be set to a value to ensure that no torque slip occurs between theflywheel 109 and the generator disk 111.

In FIG. 12, as the rectangular magnet 301 on the generator disk 111begins to rotate out of the compressed magnetic field position and awayfrom the flywheel 109, the north pole of the rectangular magnet 301 isstrongly pushed away by the repulsion force of the north pole of thetrailing driver magnet 102 on the flywheel 109 and by the magneticdecompression (i.e., spring back) of the previously compressed north andsouth fields in the MFP along the circumferential surface S (in FIG. 9)of the flywheel 109. The spring back force (i.e., magnetic decompressionforce) of the north pole in the MFP provides added repulsion to therectangular magnet 301 of the generator disk 111 as the rectangularmagnet 301 moves away from the flywheel 109.

Next, another initial magnetic compression process is started, as shownin FIG. 10, and the cycle of magnetic compression and decompressionrepeats. Thus, rotational movement of the flywheel 109 and the generatordisk 111 continues.

FIG. 14 is a layout diagram of another exemplary flywheel according tothe present invention. In FIG. 14, a flywheel 209 may include all of theabove-described features of the flywheel 109 (in FIGS. 1A-C), but mayinclude suppressor magnets 208 disposed from the circumferential surfaceS of the flywheel 209 by a distance X. For example, the distance X maybe less that a depth of the first grooves 101, and may be disposedbetween adjacent backing plates 203. Similar to the relative angulardisplacements α and β of the driver and suppressor magnets 102 and 301,the relative positioning of the suppressor magnets 208 may be disposedbetween the driver magnets 102. Thus, the suppressor magnets 208 mayfurther displace the south magnetic fields of the driver magnets 102transmitted by the backing plates 203 toward the center C of theflywheel 209. Moreover, the different exemplary driver magnets of FIGS.4-7 may be incorporated into the flywheel 209 of FIG. 14.

FIG. 15 is a layout diagram of another exemplary flywheel according tothe present invention. In FIG. 15, a flywheel 309 may include all of theabove-described features of the flywheel 109 (in FIGS. 1A-C), but mayinclude suppressor magnets 308 disposed from an end portion of thebacking plates 203 by a distance X. In addition, the suppressor magnets308 may be placed along a centerline of the driver magnets 102. Thus,the suppressor magnets 208 may further displace the south magneticfields of the driver magnets 102 transmitted by the backing plates 203toward the center C of the flywheel 309. Moreover, the differentexemplary driver magnets of FIGS. 4-7 may be incorporated into theflywheel 309 of FIG. 15.

FIG. 16 is a layout diagram of another exemplary flywheel according tothe present invention. In FIG. 16, a flywheel 409 may include all of theabove-described features of the flywheel 109 (in FIGS. 1A-C), but mayinclude a suppressor magnet ring 408 concentrically disposed with thecenter C of the flywheel 409. Thus, the suppressor magnet ring 408 mayfurther displaces the south magnetic fields of the driver magnets 102transmitted by the backing plates 203 toward the center C of theflywheel 409. Moreover, the different exemplary driver magnets of FIGS.4-7 may be incorporated into the flywheel 409 of FIG. 16.

FIG. 17 is a schematic diagram of an exemplary system using the torqueconverter according to the present invention. In FIG. 17, a system forgenerating power using the torque converted configuration of the presentinvention may include a motor 105 powered by a power source 101 using avariable frequency motor control drive 103 to rotatably drive a shaft407 coupled to the flywheel 109, as well as any of the flywheels ofFIGS. 1 and 14-16. In addition, the generator disk 111 may be coupled toa drive shaft 113, wherein rotation of the generator disk 111 will causerotation of the drive shaft 113. For example, a longitudinal axis of thedrive shaft 113 may be disposed perpendicular to a longitudinal axis ofthe drive shaft 107.

In FIG. 17, the drive shaft 113 may be coupled to a rotor 119 of anelectrical generator comprising a plurality of stators 117. An exemplarygenerator is disclosed in U.S. patent application Ser. No. 10/973,825,which is hereby incorporated by reference in its entirety. Specifically,the rotor 119 may include an even number of magnets, and each of thestators 117 may include an odd number of coils, wherein each of thecoils includes an amorphous core. The amorphous cores do not produce anyheat during operation of the electrical generator. Rotation of the rotor119 may cause the electrical generator to produce an alternating currentoutput to a variable transformer 121, and the output of the variabletransformer 121 may be provided to a load 123.

FIG. 18 is a schematic diagram of another exemplary system using thetorque converter according to the present invention. In FIG. 18, aplurality of the generator disks 1111 may be clustered around and drivenby a single flywheel 109, as well as any of the flywheels of FIGS. 1 and14-16, wherein the generator disks 111 may each be coupled to ACgenerators similar to the configuration shown in FIG. 17.

The present invention may be modified for application to mobile powergeneration source systems, as drive systems for application in stealthtechnologies, as an alternative for variable speed direct drive systems,as drive systems for pumps, fans, and HVAC systems. Moreover, thepresent invention may be modified for application to industrial,commercial, and residential vehicles requiring frictionless, gearless,and/or fluidless transmissions. Furthermore, the present invention maybe modified for application in frictionless fluid transmission systemsthrough pipes that require driving of internal impeller systems.Furthermore, the present invention may be modified for application inonboard vehicle battery charging systems, as well as power systems foraircraft, including force transmission systems for aircraft fans andpropellers.

In addition, the present invention may be modified for application inzero or low gravity environments. For example, the present invention maybe applied for use as electrical power generations systems for spacestations and interplanetary vehicles.

It will be apparent to those skilled in the art that variousmodifications and variations can be made in the torque converter andsystem using the same of the present invention without departing fromthe spirit or scope of the inventions. Thus, it is intended that thepresent invention covers the modifications and variations of thisinvention provided they come within the scope of the appended claims andtheir equivalents.

1-28. (canceled)
 29. A torque converter device transferring rotationalmotion from a first body rotatable about first axis to a second bodyrotatable about a second axis angularly offset with respect to the firstaxis, the first and second bodies separated by a gap, one of the firstand second bodies comprising: a first plurality of radially mountedmagnets; a plurality of backing plates, each disposed adjacent toinnermost end portions of the first plurality of magnets; and a magneticring equally disposed apart from each of the backing plates, wherein thebacking plates are disposed between the first plurality of radiallymounted magnets and the magnetic ring.
 30. The device according to claim29, wherein the magnetic ring displaces magnetic fields of the firstplurality of magnets toward a center of the one of the first and secondbodies.
 31. A method of transferring rotational motion from a first bodyrotatable about a first axis to a second body rotatable about a secondaxis angularly offset with respect to the first axis, comprising:compressing magnetic fields of a first plurality of magnets radiallymounted in the first body using at least one of a second plurality ofmagnets mounted in the second body; and decompressing the compressedmagnetic fields of the first plurality of magnets to transfer therotational motion of the first body to the second body.
 32. The methodaccording to claim 31, wherein the step of compressing the magneticfields includes placing magnetic field lines of the at least one of asecond plurality of magnets within magnetic field lines of adjacent onesof the first plurality of magnets along a shear plane of the at leastone of a second plurality of magnets and the adjacent ones of the firstplurality of magnets.
 33. The method according to claim 31, wherein thestep of decompressing the magnetic fields includes disengaging magneticfield lines of the at least one of a second plurality of magnets frommagnetic field lines of adjacent ones of the first plurality of magnetsalong a shear plane of the at least one of a second plurality of magnetsand the adjacent ones of the first plurality of magnets.
 34. The methodaccording to claim 33, wherein the step of decompressing magnetic fieldsincludes a third plurality of magnets mounted in the second body toprovide a repulsive force to the at least one of a second plurality ofmagnets.
 35. The method according to claim 31, wherein the first andsecond bodies are separated by a gap.
 36. The method according to claim31, wherein the first axis and the second axis are coplanar.
 37. Themethod according to claim 31, wherein the steps of compressing anddecompressing the magnetic fields includes an interface between the atleast one of a second plurality of magnets and adjacent ones of thefirst plurality of magnets.
 38. The method according to claim 37,wherein a centerline of the at least one of the second plurality magnetsand a centerline of the adjacent ones of the first plurality of magnetsare parallel.
 39. The method according to claim 38, wherein thecenterline of the at least one of the second plurality magnets and thecenterline of the adjacent ones of the first plurality of magnets areoffset from each other.
 40. The method according to claim 38, whereinthe centerline of the at least one of the second plurality magnets andthe centerline of the adjacent ones of the first plurality of magnetsare coincident.
 41. The method according to claim 37, wherein theinterface includes different geometries.
 42. The method according toclaim 41, wherein the different geometries include a cylindrical surfaceof the adjacent ones of the first plurality of magnets and planarsurfaces of the at least one of a second plurality of magnets.
 43. Asystem for generating electrical power, comprising: a motor; a flywheelrotating about a first axis, the flywheel including: a first bodyportion having a first radius from a circumferential surface and a firstradius of curvature; a first plurality of magnets mounted in the firstbody portion, each having first ends disposed from the circumferentialsurface of the first body portion, and each of the first ends of firstplurality of magnets having a radius of curvature similar to the firstradius of curvature of the first body portion; a second plurality ofmagnets mounted in the first body portion, each of the second pluralityof magnets being disposed from the circumferential surface of the firstbody portion; and a generator disk rotatable about a second axisangularly offset with respect to the first axis, the generator diskincluding: a second body portion; and a third plurality of magnetswithin the second body portion magnetically coupled to the first andsecond pluralities of magnets; and at least one electrical generatorcoupled to the at least one generator disk.
 44. The system according toclaim 43, wherein one of the first and second bodies causes rotationmotion about the first axis and the second axis.
 45. The systemaccording to claim 44, wherein the rotation include compressing magneticfields of the first plurality of magnets using at least one of thesecond plurality of magnets, and decompressing the compressed magneticfields of the first plurality of magnets to transfer the rotationalmotion of the first body to the second body.
 46. The system according toclaim 45, wherein the compressing the magnetic fields includes placingmagnetic field lines of the at least one of a second plurality ofmagnets within magnetic field lines of adjacent ones of the firstplurality of magnets along a shear plane of the at least one of a secondplurality of magnets and the adjacent ones of the first plurality ofmagnets.
 47. The system according to claim 45, wherein the decompressingthe magnetic fields includes disengaging magnetic field lines of the atleast one of a second plurality of magnets from magnetic field lines ofadjacent ones of the first plurality of magnets along a shear plane ofthe at least one of a second plurality of magnets and the adjacent onesof the first plurality of magnets.
 48. The system according to claim 45,wherein the steps of compressing and decompressing the magnetic fieldsincludes an interface between the at least one of a second plurality ofmagnets and adjacent ones of the first plurality of magnets.
 49. Thesystem according to claim 48, wherein the interface includes differentgeometries.
 50. The system according to claim 48, wherein the differentgeometries include a cylindrical surface of the adjacent ones of thefirst plurality of magnets and planar surfaces of the at least one of asecond plurality of magnets.
 51. The system according to claim 43,wherein the first and second bodies are separated by a gap.
 52. Thesystem according to claim 43, wherein the first axis and the second axisare coplanar. 53-61. (canceled)